16 research outputs found
Magnetostatic Interactions in Self-Assembled Co<sub><i>x</i></sub>Ni<sub>1–<i>x</i></sub>Fe<sub>2</sub>O<sub>4</sub>/BiFeO<sub>3</sub> Multiferroic Nanocomposites
Self-assembled
vertically aligned oxide nanocomposites consisting
of magnetic pillars embedded in a ferroelectric matrix have been proposed
for logic devices made from arrays of magnetostatically interacting
pillars. To control the ratio between the nearest neighbor interaction
field and the switching field of the pillars, the pillar composition
Co<sub><i>x</i></sub>Ni<sub>1–<i>x</i></sub>Fe<sub>2</sub>O<sub>4</sub> was varied over the range 0 ≤ <i>x</i> ≤ 1, which alters the magnetoelastic and magnetocrystalline
anisotropy and the saturation magnetization. Nanocomposites were templated
into square arrays of pillars in which the formation of a “checkerboard”
ground state after ac-demagnetization indicated dominant magnetostatic
interactions. The effect of switching field distribution in disrupting
the antiparallel nearest neighbor configuration was analyzed using
an Ising model and compared with experimental results
Thickness-Dependent Double-Epitaxial Growth in Strained SrTi<sub>0.7</sub>Co<sub>0.3</sub>O<sub>3−δ</sub> Films
Perovskite-structured
SrTi<sub>0.7</sub>Co<sub>0.3</sub>O<sub>3−δ</sub> (STCo)
films of varying thicknesses were grown on SrTiO<sub>3</sub>(001)
substrates using pulsed laser deposition. Thin films grow with a cube-on-cube
epitaxy, but for films exceeding a critical thickness of about 120
nm, a double-epitaxial microstructure was observed, in which (110)-oriented
crystals nucleated within the (001)-oriented STCo matrix, both orientations
being epitaxial with the substrate. The crystal structure, strain
state, and magnetic properties are described as a function of film
thickness. Both the magnetic moment and the coercivity show maxima
at the critical thickness. The formation of a double-epitaxial microstructure
provides a mechanism for strain relief in epitaxially mismatched films
Ordered Nanoscale Archimedean Tilings of a Templated 3‑Miktoarm Star Terpolymer
The directed self-assembly of 3-miktoarm star terpolymer
chains
(polyisoprene-<i>arm</i>-polystyrene-<i>arm</i>-polyferrocenylethylmethylsilane (3 μ-ISF)) into 2D Archimedean
tilings is described. A morphological change from (4.8<sup>2</sup>) to (6<sup>3</sup>) tiling is reported in the 3 μ-ISF thin
film blended with PS homopolymer when a greater swelling of PI is
achieved during the solvent annealing process. Highly oriented (4.8<sup>2</sup>) tilings were produced by templating the self-assembled three
colored structures in blended thin films. The use of (4.8<sup>2</sup>) and (6<sup>3</sup>) tilings as nanolithographic masks to transfer
square and triangular hole arrays into the substrate is also demonstrated
Optimizing Topographical Templates for Directed Self-Assembly of Block Copolymers via Inverse Design Simulations
An inverse design algorithm has been
developed that predicts the
necessary topographical template needed to direct the self-assembly
of a diblock copolymer to produce a given complex target structure.
The approach is optimized by varying the number of topographical posts,
post size, and block copolymer volume fraction to yield a template
solution that generates the target structure in a reproducible manner.
The inverse algorithm is implemented computationally to predict post
arrangements that will template two different target structures and
the predicted templates are tested experimentally with a polydimethylsiloxane-<i>b</i>-polystyrene block copolymer. Simulated and experimental
results show overall very good agreement despite the complexity of
the patterns. The templates determined from the model can be used
in developing simpler design rules for block copolymer directed self-assembly
The Spatial Resolution Limit for an Individual Domain Wall in Magnetic Nanowires
Magnetic
nanowires are the foundation of several promising nonvolatile
computing devices, most notably magnetic racetrack memory and domain
wall logic. Here, we determine the analog information capacity in
these technologies, analyzing a magnetic nanowire containing a single
domain wall. Although wires can be deliberately patterned with notches
to define discrete positions for domain walls, the line edge roughness
of the wire can also trap domain walls at dimensions below the resolution
of the fabrication process, determining the fundamental resolution
limit for the placement of a domain wall. Using a fractal model for
the edge roughness, we show theoretically and experimentally that
the analog information capacity for wires is limited by the self-affine
statistics of the wire edge roughness, a relevant result for domain
wall devices scaled to regimes where edge roughness dominates the
energy landscape in which the walls move
Morphology Control in Block Copolymer Films Using Mixed Solvent Vapors
Solvent vapor annealing of block copolymer thin films can produce a range of morphologies different from the equilibrium bulk morphology. By systematically varying the flow rate of two different solvent vapors (toluene and <i>n</i>-heptane) and an inert gas, phase maps showing the morphology <i>versus</i> vapor pressure of the solvents were constructed for 45 kg/mol polystyrene-<i>block</i>-polydimethylsiloxane diblock copolymer films of different thicknesses. The final morphology was correlated with the swelling of the block copolymer and homopolymer films and the solvent vapor annealing conditions. Self-consistent field theory is used to model the effects of solvent swelling. These results provide a framework for predicting the range of morphologies available under different solvent vapor conditions, which is important in lithographic applications where precise control of morphology and critical dimensions are essential
Aligned Sub-10-nm Block Copolymer Patterns Templated by Post Arrays
Self-assembly of block copolymer films can generate useful periodic nanopatterns, but the self-assembly needs to be templated to impose long-range order and to control pattern registration with other substrate features. We demonstrate here the fabrication of aligned sub-10-nm line width patterns with a controlled orientation by using lithographically formed post arrays as templates for a 16 kg/mol poly(styrene-block-dimethylsiloxane) (PS-<i>b</i>-PDMS) diblock copolymer. The in-plane orientation of the block copolymer cylinders was controlled by varying the spacing and geometry of the posts, and the results were modeled using 3D self-consistent field theory. This work illustrates how arrays of narrow lines with specific in-plane orientation can be produced, and how the post height and diameter affect the self-assembly
Templated Self-Assembly of a PS-<i>Branch</i>-PDMS Bottlebrush Copolymer
The
self-assembly of block copolymers (BCPs) with novel architectures
offers tremendous opportunities in nanoscale patterning and fabrication.
Here, the thin film morphology, annealing kinetics, and topographical
templating of an unconventional Janus-type “PS-<i>branch</i>-PDMS” bottlebrush copolymer (BBCP) are described. In the
Janus-type BBCP, each segment of the bottlebrush backbone connects
two immiscible side chain blocks. Thin films of a Janus-type BBCP
with <i>M</i><sub>n</sub> = 609 kg/mol exhibited 22 nm period
cylindrical microdomains with long-range order under solvent vapor
annealing, and the effects of as-cast film thickness, solvent vapor
pressure, and composition of the binary mixture of solvent vapors
are described. The dynamic self-assembly process was characterized
using in situ grazing-incidence X-ray scattering. Templated self-assembly
of the BBCP within lithographically patterned substrates was demonstrated,
showing distinct pattern orientation and dimensions that differ from
conventional BCPs. Self-consistent field theory is used to elucidate
details of the templated self-assembly behavior within confinement
Interfacial Energy-Controlled Top Coats for Gyroid/Cylinder Phase Transitions of Polystyrene-<i>block</i>-polydimethylsiloxane Block Copolymer Thin Films
Block copolymers
(BCPs) with a high Flory–Huggins interaction parameter (χ)
can form well-defined sub-10 nm periodic structures and can be used
as a template for fabrication of various functional nanostructures.
However, the large difference of surface energy between the blocks
commonly found in high-χ BCPs makes it challenging to stabilize
a useful gyroid morphology in thin film form. Here, we used an interfacial-energy-tailored
top-coat on a blended film of a polystyrene-<i>block</i>-polydimethylsiloxane (PS-<i>b</i>-PDMS) BCP and a low-molecular-weight
PDMS homopolymer with a hydrophilic end functional group. The top
coat consisted of a random mixture of 40% hydrolyzed poly(vinyl acetate)-<i>random</i>-poly(vinly alcohol) (PVA-<i>r</i>-PVAc,
PVA40) and PVAc homopolymer. At the optimized top-coat composition,
gyroid nanostructures with sub-10 nm strut width were achieved down
to ∼125 nm film thickness, which is only 3 times the lattice
parameter of the gyroid structure. This is in marked contrast with
a mixed morphology of gyroid and cylinders obtained for other compositions
of the top coat. Self-consistent field theoretic simulations were
used to understand the effect of the interfacial energy between the
top coat and BCP/homopolymer blends on the phase transition behavior
of the BCP/homopolymer films
Magnetic Phase Formation in Self-Assembled Epitaxial BiFeO<sub>3</sub>–MgO and BiFeO<sub>3</sub>–MgAl<sub>2</sub>O<sub>4</sub> Nanocomposite Films Grown by Combinatorial Pulsed Laser Deposition
Self-assembled epitaxial BiFeO<sub>3</sub>–MgO and BiFeO<sub>3</sub>–MgAl<sub>2</sub>O<sub>4</sub> nanocomposite thin films
were grown on SrTiO<sub>3</sub> substrates by pulsed laser deposition.
A two-phase columnar structure was observed for BiFeO<sub>3</sub>–MgO
codeposition within a small window of growth parameters, in which
the pillars consisted of a magnetic spinel phase (Mg,Fe)<sub>3</sub>O<sub>4</sub> within a BiFeO<sub>3</sub> matrix, similar to the growth
of BiFeO<sub>3</sub>–MgFe<sub>2</sub>O<sub>4</sub> nanocomposites
reported elsewhere. Further, growth of a nanocomposite with BiFeO<sub>3</sub>–(CoFe<sub>2</sub>O<sub>4</sub>/MgO/MgFe<sub>2</sub>O<sub>4</sub>), in which the minority phase was grown from three
different targets, gave spinel pillars with a uniform (Mg,Fe,Co)<sub>3</sub>O<sub>4</sub> composition due to interdiffusion during growth,
with a bifurcated shape from the merger of neighboring pillars. BiFeO<sub>3</sub>–MgAl<sub>2</sub>O<sub>4</sub> did not form a well-defined
vertical nanocomposite in spite of having lower lattice mismatch,
but instead formed a two-phase film with in which the spinel phase
contained Fe. These results illustrate the redistribution of Fe between
the oxide phases during oxide codeposition to form a ferrimagnetic
phase from antiferromagnetic or nonmagnetic targets